for the full range of \(t\)  along the ERG trajectory. These masses are even greater in the regime \(f > \Lambda ^2\)  considered in [1]}.
This makes the whole setup of the ERG in the theory in [1]} questionable, regardless of its relation to theories with non-linear supersymmetry. In this evaluation of masses we are using their own eq. (3.7) in [1]}. But the Polchinski flow equation [4]}, [5]}
for a Wilsonian action approach is based on a restriction on the allowed momenta of the form
\(p^2 \le \mu ^2 \le \Lambda ^2 \ .\) 
